of
the ray of light between the two sheets of glass. Such an instrument is
a simple form of the polariscope. More frequently two prisms of Iceland
Spar cut and mounted in a particular way are used to polarise and
analyse the light; such prisms are called "Nicol's prisms"; the prisms
are mounted so as to be capable of complete rotation with regard to one
another, and there are two positions in the complete revolution of
maximum extinction of light; when the prisms are in one of these two
positions, they are said to be "crossed." Now a singly-refracting body
placed between crossed Nicol's prisms allows no light to pass whatever
the position of the body, but in the examination of a gem we must use
two or even three positions to make sure we are not dealing with a
doubly refracting substance placed with the optic axis in the axis of
the instrument. In examining a gem it must be first placed resting in
the carrier on its small back facet, so as to give the light every
opportunity of being transmitted through the stone. If there is a
possibility that total internal reflection is preventing the light
reaching the eye, we may overcome the possible fallacy by immersing the
gem in a liquid of similar refractive index; for this purpose methylene
iodide or mono-bromo-naphthalene may be used. When a doubly-refracting
stone is placed in the right position, we shall find on rotating it
that there are four positions in the 360° in which there is maximum
lightness, due to the light being so altered in its passage through the
gem that it can pass through the analyser.
One
other possible fallacy remains to be mentioned. Some singly-refracting
substances show what is known as anomalous double refraction ; this is
due to strains set up